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Design and performance of the field cage for the XENONnT experiment
Stockholm University, Faculty of Science, Department of Physics. Stockholm University, Faculty of Science, The Oskar Klein Centre for Cosmo Particle Physics (OKC).ORCID iD: 0000-0003-1331-2890
Stockholm University, Faculty of Science, Department of Physics. Stockholm University, Faculty of Science, The Oskar Klein Centre for Cosmo Particle Physics (OKC).ORCID iD: 0000-0001-9984-4411
Stockholm University, Faculty of Science, Department of Physics. Stockholm University, Faculty of Science, The Oskar Klein Centre for Cosmo Particle Physics (OKC). Stockholm Univ, Oskar Klein Ctr, Dept Phys, AlbaNova, S-10691 Stockholm, Sweden.ORCID iD: 0000-0002-4664-5504
Stockholm University, Faculty of Science, The Oskar Klein Centre for Cosmo Particle Physics (OKC). Stockholm University, Faculty of Science, Department of Physics.
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Number of Authors: 1642024 (English)In: European Physical Journal C, ISSN 1434-6044, E-ISSN 1434-6052, Vol. 84, no 2, article id 138Article in journal (Refereed) Published
Abstract [en]

The precision in reconstructing events detected in a dual-phase time projection chamber depends on an homogeneous and well understood electric field within the liquid target. In the XENONnT TPC the field homogeneity is achieved through a double-array field cage, consisting of two nested arrays of field shaping rings connected by an easily accessible resistor chain. Rather than being connected to the gate electrode, the topmost field shaping ring is independently biased, adding a degree of freedom to tune the electric field during operation. Two-dimensional finite element simulations were used to optimize the field cage, as well as its operation. Simulation results were compared to 83mKr calibration data. This comparison indicates an accumulation of charge on the panels of the TPC which is constant over time, as no evolution of the reconstructed position distribution of events is observed. The simulated electric field was then used to correct the charge signal for the field dependence of the charge yield. This correction resolves the inconsistent measurement of the drift electron lifetime when using different calibrations sources and different field cage tuning voltages.

Place, publisher, year, edition, pages
2024. Vol. 84, no 2, article id 138
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Subatomic Physics
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URN: urn:nbn:se:su:diva-226992DOI: 10.1140/epjc/s10052-023-12296-yISI: 001159991600006Scopus ID: 2-s2.0-85195205079OAI: oai:DiVA.org:su-226992DiVA, id: diva2:1842267
Available from: 2024-03-04 Created: 2024-03-04 Last updated: 2025-02-14Bibliographically approved

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Antochi, Vasile C.Conrad, JanRosso, Andrea GalloJoy, AshleyMahlstedt, JörnTan, Pueh-Leng

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European Physical Journal C
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